Manuscript Hawk04-A@1 · Hawk04-A.tex · theorem · 526092ba
Theorem: Reference-preserving finite regulator
A regulated interacting microscopic application › Finite approximation of the complete dilation · lines 1257–1367 · proof included or linked
Hawk04-A@1#thm:regulator, Hawk04-A@1#eq:regulator, Hawk04-A@1#eq:selection
At fixed , every finite observation interval and finite packet family admit a finite-dimensional prepared isometry such that
uniformly for . The same bound holds for both complete complementary outputs after their common embeddings.
For , it suffices to choose and a mesh with
when . Then .
Proof. In interaction picture,
On sectors containing at most particles,
An -fold product acting on bath vacuum has norm at most . The ordered integration simplex has volume . The vacuum Dyson term is consequently bounded by
The bound is uniform over source, carrier, and reference inputs.
The series converges, also after multiplication by any fixed power of . Since each term has occupation at most , it converges in every fixed particle-number graph norm. On these vectors the differentiated series satisfies the Schrödinger equation; uniqueness for the self-adjoint Hamiltonian identifies it with the actual evolution.
The evolution generated by , on its projected space, has the same Dyson terms through order . Inserted projections are contractions, so the difference of the two prepared isometries is at most .
Partition into intervals of width at most , and replace frequency multiplication by its bin midpoint value . Then
Duhamel's formula adds at most .
For an exact finite active-mode realization of this discretized model, take
It contains all coupling vectors and the complete packet space, and is invariant under . Its orthogonal complement remains vacuum. Thus the occupation-truncated dynamics on is finite dimensional.
The total-occupation subspace is embedded into the product
This is an embedding, not an assertion that the total cutoff itself factorizes. The source and carrier are retained. Apply Lemma lem:isometry and partial trace.
For the explicit selection, let . The first condition gives
The subsequent tail-term ratios are at most , so . The second condition makes ; the mesh condition bounds the remaining term by .
Displayed formulas in this passage
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